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Limitations of Bohr's Theory
Dr. Mithil Fal Desai
Shree Mallikarjun and Shri
Chetan Manju Desai College
Canacona Goa
Background
J. Dalton
1803
J. J.
Thomson
1904
E. Rutherford
1911
N. Bohr
1913
Neil Bohr postulated
 Electron does not radiate energy as it moves in a particular orbit.
 Electron can move from one orbit to another absorbing or radiating
energy.
 Centrifugal force in which electron orbits is equal to electrostatic force,
thus electron remains in orbit.
e-
Calculating Bohr radius
e-
Electron to remain in orbit
𝑪𝒆𝒕𝒓𝒊𝒇𝒖𝒈𝒂𝒍 𝒇𝒐𝒓𝒄𝒆
= 𝑬𝒍𝒆𝒄𝒕𝒓𝒐𝒔𝒕𝒂𝒕𝒊𝒄 𝒇𝒐𝒓𝒄𝒆
𝑚𝑣2
𝑟
=
𝑍𝑒2
4𝜋𝜀°𝑟2 …………..1
Where,
r is radius of atom, mass of electron m =
9.1091 X 10-31 Kg; charge on electron e =
1.60210 X 10-19 C; vacuum permittivity
of vacuum εo = 8.854185 X 10-12J-1m-1C2
r
Calculating Bohr radius
According to Plank ‘Energy is discrete’: only certain energy levels are
possible which integral multiple of h/2𝜋 ( of n a whole number 0, 1, 2, 3…)
Plank constant h = 6.6262 X10-34Js
𝐴𝑛𝑔𝑢𝑙𝑎𝑟 𝑚𝑜𝑚𝑒𝑛𝑡𝑢𝑚 = 𝐸𝑙𝑒𝑐𝑡𝑟𝑜𝑠𝑡𝑎𝑡𝑖𝑐 𝑓𝑜𝑟𝑐𝑒
𝑚𝑣𝑟 =
𝑛ℎ
2𝜋
………………..2
From 1 and 2
𝑟 =
𝑛2ℎ2ε°
𝜋𝑍𝑚𝑒2
For Hydrogen, Z = 1, than for
n=1; r = 1 X 0.0529 nm
n=2; r = 22 X 0.0529 nm
e-
Energy of orbit and energy of
electronic transition
For energy we can consider equation 1
𝐸 = −
1
2
𝑚𝑣2
= −
𝑍2𝑒4𝑚
8 𝑛2ℎ2ε°
2………………..3
Difference in energy (ΔE) of two orbits
𝐸2 − 𝐸1 = −
𝑍2
𝑒4
𝑚
8𝑛2
2ℎ2ε°
2 − (−
𝑍2
𝑒4
𝑚
8𝑛1
2ℎ2ε°
2)
ΔE =
𝑍2𝑒4𝑚
8ℎ2ε°
2 (
1
𝑛1
2 −
1
𝑛2
2) ………………..4
Energy of orbit and energy of
electronic transition
𝐸 = ℎ𝑣 = ℎṽ𝐶
ṽ = 𝑤𝑎𝑣𝑒𝑛𝑢𝑚𝑏𝑒𝑟
Then,
ṽ =
𝑍2𝑒4𝑚
8ℎ3ε°
2𝐶
(
1
𝑛1
2 −
1
𝑛2
2)
ṽ = 𝑅 (
1
𝑛1
2 −
1
𝑛2
2)
R= Rydberg constant =1.0973 X 107 m-1
Bohr orbit of hydrogen atom and
spectral series
Series name n1 n2 ʎ nm Electromagn
etic radiation
Lyman 1 2,3,4,5… 91.2-121.6 UV
Balmer 2 3,4,5,6… 383.5-656.2 Visible
Paschen 3 4,5,6,7… 954.6-
1875.0
Infrared
Brackett 4 5,6,7,8… 2630-4050 Infrared
Pfund 5 6,….. 7400 infrared
Limitations
• Spectral lines is a collection of several lines very
close together.
• does not spectral series for the atoms having a
more number of electrons.
• Bohr theory does not explain the use of the
principle of quantization of energy
• Bohr assumes electrons are at a fixed point
• No justification of the Zeeman effect or Stark
effect.
Bohr's Theory
• Why electron does not slow down as it moves in orbit?
• Why circular path it follows?
• Why electron does not collide with nucleus as electron
is negative and nucleus positive.
e-

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Limitations of Bohr's theory

  • 1. Limitations of Bohr's Theory Dr. Mithil Fal Desai Shree Mallikarjun and Shri Chetan Manju Desai College Canacona Goa
  • 2. Background J. Dalton 1803 J. J. Thomson 1904 E. Rutherford 1911 N. Bohr 1913
  • 3. Neil Bohr postulated  Electron does not radiate energy as it moves in a particular orbit.  Electron can move from one orbit to another absorbing or radiating energy.  Centrifugal force in which electron orbits is equal to electrostatic force, thus electron remains in orbit. e-
  • 4. Calculating Bohr radius e- Electron to remain in orbit 𝑪𝒆𝒕𝒓𝒊𝒇𝒖𝒈𝒂𝒍 𝒇𝒐𝒓𝒄𝒆 = 𝑬𝒍𝒆𝒄𝒕𝒓𝒐𝒔𝒕𝒂𝒕𝒊𝒄 𝒇𝒐𝒓𝒄𝒆 𝑚𝑣2 𝑟 = 𝑍𝑒2 4𝜋𝜀°𝑟2 …………..1 Where, r is radius of atom, mass of electron m = 9.1091 X 10-31 Kg; charge on electron e = 1.60210 X 10-19 C; vacuum permittivity of vacuum εo = 8.854185 X 10-12J-1m-1C2 r
  • 5. Calculating Bohr radius According to Plank ‘Energy is discrete’: only certain energy levels are possible which integral multiple of h/2𝜋 ( of n a whole number 0, 1, 2, 3…) Plank constant h = 6.6262 X10-34Js 𝐴𝑛𝑔𝑢𝑙𝑎𝑟 𝑚𝑜𝑚𝑒𝑛𝑡𝑢𝑚 = 𝐸𝑙𝑒𝑐𝑡𝑟𝑜𝑠𝑡𝑎𝑡𝑖𝑐 𝑓𝑜𝑟𝑐𝑒 𝑚𝑣𝑟 = 𝑛ℎ 2𝜋 ………………..2 From 1 and 2 𝑟 = 𝑛2ℎ2ε° 𝜋𝑍𝑚𝑒2 For Hydrogen, Z = 1, than for n=1; r = 1 X 0.0529 nm n=2; r = 22 X 0.0529 nm e-
  • 6. Energy of orbit and energy of electronic transition For energy we can consider equation 1 𝐸 = − 1 2 𝑚𝑣2 = − 𝑍2𝑒4𝑚 8 𝑛2ℎ2ε° 2………………..3 Difference in energy (ΔE) of two orbits 𝐸2 − 𝐸1 = − 𝑍2 𝑒4 𝑚 8𝑛2 2ℎ2ε° 2 − (− 𝑍2 𝑒4 𝑚 8𝑛1 2ℎ2ε° 2) ΔE = 𝑍2𝑒4𝑚 8ℎ2ε° 2 ( 1 𝑛1 2 − 1 𝑛2 2) ………………..4
  • 7. Energy of orbit and energy of electronic transition 𝐸 = ℎ𝑣 = ℎṽ𝐶 ṽ = 𝑤𝑎𝑣𝑒𝑛𝑢𝑚𝑏𝑒𝑟 Then, ṽ = 𝑍2𝑒4𝑚 8ℎ3ε° 2𝐶 ( 1 𝑛1 2 − 1 𝑛2 2) ṽ = 𝑅 ( 1 𝑛1 2 − 1 𝑛2 2) R= Rydberg constant =1.0973 X 107 m-1
  • 8. Bohr orbit of hydrogen atom and spectral series Series name n1 n2 ʎ nm Electromagn etic radiation Lyman 1 2,3,4,5… 91.2-121.6 UV Balmer 2 3,4,5,6… 383.5-656.2 Visible Paschen 3 4,5,6,7… 954.6- 1875.0 Infrared Brackett 4 5,6,7,8… 2630-4050 Infrared Pfund 5 6,….. 7400 infrared
  • 9. Limitations • Spectral lines is a collection of several lines very close together. • does not spectral series for the atoms having a more number of electrons. • Bohr theory does not explain the use of the principle of quantization of energy • Bohr assumes electrons are at a fixed point • No justification of the Zeeman effect or Stark effect.
  • 10. Bohr's Theory • Why electron does not slow down as it moves in orbit? • Why circular path it follows? • Why electron does not collide with nucleus as electron is negative and nucleus positive. e-